The incommensurate composite Y<sub> <i>x</i> </sub>Os<sub>4</sub>B<sub>4</sub> (<i>x</i> = 1.161)

Y<sub>x</sub>Os<sub>4</sub>B<sub>4</sub> (x = 1.161) crystallizes as a tetragonal incommensurate composite of columns of Y atoms extending along [001] in an Os<sub>4</sub>B<sub>4</sub> framework. The structure was refined using the superspace approach. The basic structure of the Y subsystem can be idealized as having I4/mmm symmetry, with a crystallographically unique Y atom located on the 4/mmm position. The actual superspace symmetry is P4<sub>2</sub>/nmc(00σ<sub>3</sub>)s0s0. The Y atoms feature only subtle positional modulation in the [001] direction. The Os<sub>4</sub>B<sub>4</sub> subsystem [P4<sub>2</sub>/ncm(00σ<sub>3</sub>)00ss superspace symmetry] is built of columns of edge-sharing Os<sub>4</sub> tetrahedra extending along [001] and B<sub>2</sub> dumbbells. The Os<sub>4</sub> tetrahedra feature pronounced positional modulation with a distinct variation of the Os-Os bond lengths. Modulation of the B<sub>2</sub> dumbbells is best described as a rotation about the [001] axis.

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Publication Details

Journal
Acta Crystallographica Section B Structural Science Crystal Engineering and Materials
Published
2024-10-31
DOI
https://doi.org/10.1107/s205252062400982x
Citations
1
Primary Topic
Magnetic Properties of Alloys
Type
article
Field-Weighted Citation Impact
0.12

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article

The incommensurate composite Y x Os4B4 (x = 1.161)

O. Sologub, Leonid Salamakha, Berthold Stöger
1 citations
Acta Crystallographica Section B Structural Science Crystal Engineering and Materials
Magnetic Properties of Alloys
0.12
article

The incommensurate composite Y x Os4B4 (x = 1.161)

O. Sologub, Leonid Salamakha, Berthold Stöger
article en
1 citations

Abstract

Y<sub>x</sub>Os<sub>4</sub>B<sub>4</sub> (x = 1.161) crystallizes as a tetragonal incommensurate composite of columns of Y atoms extending along [001] in an Os<sub>4</sub>B<sub>4</sub> framework. The structure was refined using the superspace approach. The basic structure of the Y subsystem can be idealized as having I4/mmm symmetry, with a crystallographically unique Y atom located on the 4/mmm position. The actual superspace symmetry is P4<sub>2</sub>/nmc(00σ<sub>3</sub>)s0s0. The Y atoms feature only subtle positional modulation in the [001] direction. The Os<sub>4</sub>B<sub>4</sub> subsystem [P4<sub>2</sub>/ncm(00σ<sub>3</sub>)00ss superspace symmetry] is built of columns of edge-sharing Os<sub>4</sub> tetrahedra extending along [001] and B<sub>2</sub> dumbbells. The Os<sub>4</sub> tetrahedra feature pronounced positional modulation with a distinct variation of the Os-Os bond lengths. Modulation of the B<sub>2</sub> dumbbells is best described as a rotation about the [001] axis.

Acta Crystallographica Section B Structural Science Crystal Engineering and MaterialsVol. 80(6)
TU Wien (AT)
Austrian Science Fund, Technische Universität Wien, Technische Universität Wien Bibliothek
Openalex Percentile: Top 65%
Magnetic Properties of Alloys
0.12
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